Prism film, backlight module and display device

ABSTRACT

Embodiments of the present disclosure relate to a prism film, a backlight module, and a display device. The prism film includes a substrate and a plurality of prisms on a surface of the substrate, each of the plurality of prisms having a triangular cross section, and having a first optical surface, a second optical surface, and a third optical surface that are perpendicular to the triangular cross section, wherein the first optical surface is parallel to the surface of the substrate, the first optical surface and the second optical surface form a first bottom angle, the first optical surface and the third optical surface form a second bottom angle, and at least one of the first bottom angle and the second bottom angle of the plurality of prisms gradually changes.

CROSS REFERENCE TO RELATED APPLICATIONS

This patent application claims the benefit and priority of ChinesePatent Application No. 201810272472.0 filed on Mar. 29, 2018, thedisclosure of which is incorporated by reference herein in its entiretyas part of the present application.

BACKGROUND

Embodiments of the present disclosure relate to the field of displaytechnologies, and in particular, to a prism film, a backlight module,and a display device.

The liquid crystal display panel has been developed into a maturedisplay technology and may be applied to various fields. As anapplication example, a liquid crystal display panel may be used invirtual reality (VR) display technology to present visual informationfor visual perception. By means of the imaging lens and the stereoscopicdisplay technology, the information presented on the display panel maybe perceived as real, so that a very realistic experience may beprovided.

BRIEF DESCRIPTION

Embodiments of the present disclosure provide a prism film, a backlightmodule, and a display device.

An aspect of the present disclosure provides a prism film. The prismfilm includes a substrate and a plurality of prisms on a surface of thesubstrate, each of the plurality of prisms having a triangular crosssection, and having a first optical surface, a second optical surface,and a third optical surface that are perpendicular to the triangularcross section. The first optical surface is parallel to the surface ofthe substrate, the first optical surface and the second optical surfaceform a first bottom angle, and the first optical surface and the thirdoptical surface form a second bottom angle. At least one of the firstbottom angle and the second bottom angle of the plurality of prismsgradually changes.

In an embodiment, the plurality of prisms are arranged in parallel in adirection parallel to the surface of the substrate. The first bottomangle and the second bottom angle are configured such that lightentering the prism from the second optical surface may be reflectedtoward the first optical surface by the third optical surface, and thenemerge from the first optical surface in a way of being deflected towarda center of the substrate.

In an embodiment, the direction is a direction of a horizontal componentof the light parallel to the surface of the substrate, and the at leastone of the first bottom angle and the second bottom angle of theplurality of prisms gradually increases in the direction.

In an embodiment, the first bottom angle and the second bottom angle areconfigured to satisfy the following relationship:

${\sin \; \theta \; 8} = {n*{\sin \left\lbrack {{\alpha \; 1} + {2*\alpha \; 3} - \pi + {\arcsin \; \frac{\sin \left( {{\theta \; 1} - {\alpha 1}} \right)}{n}}} \right\rbrack}}$${\arcsin \; \frac{\sin \left( {{\theta \; 1} - {\alpha 1}} \right)}{n}} > {\frac{\pi}{2} - {\alpha 1} - {\alpha \; 3}}$

wherein θ1 represents an angle, facing the substrate, between adirection of light incident on the prism and a normal to the surface ofthe substrate, n represents a refractive index of the prism, α1represents the first bottom angle, α3 indicates the second bottom angle,and θ8 represents an outgoing angle of light emerging from the firstoptical surface.

In an embodiment, the first bottom angle and the second bottom angle areconfigured such that the light incident to the third optical surface istotally reflected at the third optical surface, wherein the first bottomangle and the second bottom angle are further configured to satisfy thefollowing relationship:

${\theta \; 5} = {{\pi - {\alpha \; 1} - {\alpha \; 3} - {\arcsin \; \frac{\sin \left( {{\theta \; 1} - {\alpha 1}} \right)}{n}}} > {\arcsin \; \frac{1}{n}}}$

where θ5 represents an incident angle of the light at the third opticalsurface.

In an embodiment, the triangular cross section is an isoscelestriangular cross section.

In an embodiment, 65°≤θ1≤85°.

In an embodiment, the second bottom angle is a right angle, and thefirst bottom angle is configured such that light entering the prism fromthe first optical surface may be directly incident on the second opticalsurface, and then emerge from the second optical surface in a way ofbeing deflected toward the center of the substrate.

In an embodiment, the first bottom angle of the plurality of prismsgradually decreases from an edge of the substrate toward the center ofthe substrate.

In an embodiment, the first bottom angle is configured to satisfy thefollowing relationship:

$\delta = {{\arcsin \left\lbrack {n*{\sin \left( {{\alpha \; 1} + {\arcsin \; \frac{\sin \; \beta \; 1}{n}}} \right)}} \right\rbrack} - {\alpha \; 1}}$${{\alpha \; 1} + {\arcsin \; \frac{\sin \; \beta \; 1}{n}}} < {\arcsin \; \frac{1}{n}}$

wherein δ represents an angle between the light emerging from the secondoptical surface and a normal to the first optical surface, n representsa refractive index of the prism, α1 represents the first bottom angle,and β1 represents an incident angle of the light at the first opticalsurface.

In an embodiment, 0°≤β1≤20°.

In an embodiment, the plurality of prisms are arranged in parallel in adirection parallel to the surface of the substrate.

In an embodiment, the plurality of prisms are arranged in a form of aplurality of concentric circles.

Another aspect of the present disclosure provides a backlight module.The backlight module includes a light guide plate and a prism film on alight outgoing side of the light guide plate, for example, a prism filmprovided according to one or more embodiments of the present disclosure.

In an embodiment, the plurality of prisms are arranged in parallel alonga direction parallel to the surface of the substrate. The first bottomangle and the second bottom angle are configured such that lightentering the prism from the second optical surface may be reflectedtoward the first optical surface by the third optical surface, and thenemerge from the first optical surface in a way of being deflected towardthe center of the substrate. A side of the prism film provided with theprisms is opposite to a light outgoing side of the light guide plate,and an outgoing angle of light emerging from the light guide plateranges from about 65° to about 85°.

In an embodiment, the triangular cross section is a right triangle crosssection, and the first bottom angle is configured such that lightentering the prism from the first optical surface may be directlyincident on the second optical surface, and then emerge from the secondoptical surface in a way of being deflected toward the center of thesubstrate. A side of the prism film provided with the prism faces awayfrom the light outgoing side of the light guide plate, and the outgoingangle of the light emerging from the light guide plate ranges from 0° toabout 20°.

Another aspect of the present disclosure provides a display device. Thedisplay device includes a prism film, such as the prism film providedaccording to one or more embodiments of the present disclosure.

In an embodiment, the display device may further include a backlightmodule and a display panel. The prism film is located between a lightguide plate of the backlight module and the display panel. The pluralityof prisms are arranged in parallel in a direction parallel to a surfaceof the substrate. The first bottom angle and the second bottom angle areconfigured such that light entering the prism from the second opticalsurface may be reflected toward the first optical surface by the thirdoptical surface, and then emerge from the first optical surface in a wayof being deflected toward the center of the substrate. A side of theprism film provided with the prisms is opposite to a light outgoing sideof the light guide plate, and an outgoing angle of light emerging fromthe light guide plate ranges from about 65° to about 85°.

In an embodiment, the display device further includes a display panel.The prism film is located on a light outgoing side of the display panel.The triangular cross section is a right triangle cross section. Thefirst bottom angle is configured such that light entering the prism fromthe first optical surface may be directly incident on the second opticalsurface, and then emerge from the second optical surface in a way ofbeing deflected toward the center of the substrate. A side of the prismfilm provided with the prisms faces away from a light outgoing side ofthe display panel, and an outgoing angle of the light emerging from thelight guide plate ranges from about 0° to about 20°.

In an embodiment, the display device is a virtual reality displaydevice.

Further adaptive aspects and scopes become apparent from the descriptionprovided herein. It should be understood that various aspects of thepresent disclosure may be implemented separately or in combination withone or more other aspects. It should also be understood that thedescription in the present disclosure which is intended to be merelydescribed in the specific embodiments is not intended to limit the scopeof the present disclosure.

BRIEF DESCRIPTION OF THE DRAWINGS

The accompanying drawings set forth herein are merely for the purpose ofdescribing the selected embodiments, are not all possibleimplementations and are not intended to limit the scope of the presentdisclosure, in which:

FIG. 1A shows a schematic diagram of an optical path of light exitingfrom a display screen not matching a desired optical path of a VR;

FIG. 1B shows a schematic diagram of the optical path of light exitingfrom the display screen matching the desired optical path of the VR;

FIG. 2 shows a cross-sectional view of a prism film provided accordingto an example embodiment of the present disclosure;

FIG. 3 is a schematic diagram showing the effect of the prism filmprovided by the embodiment shown in FIG. 2 on parallel light incidentthereon;

FIGS. 4A and 4B schematically show two example optical paths of lighttransmitting through a prism film in the embodiment shown in FIG. 2,respectively;

FIG. 5A shows a simulated optical path of a virtual reality displaydevice with the prism film of the embodiment shown in FIG. 2;

FIG. 5B shows a simulated optical path of a virtual reality displaydevice with the prism film having the prisms of the same bottom angle;

FIG. 6 shows a cross-sectional view of a prism film provided accordingto another example embodiment of the present disclosure;

FIG. 7 is a schematic diagram showing the effect of the prism filmprovided by the embodiment shown in FIG. 6 on the parallel lightincident perpendicular thereon;

FIGS. 8A and 8B show schematic diagrams of two example arrangements ofprisms on a substrate, respectively;

FIG. 9 shows an example optical path of light transmitting through theprism film in the embodiment shown in FIG. 6;

FIG. 10A shows a simulated optical path of a virtual reality displaydevice with the prism film of the embodiment shown in FIG. 6;

FIG. 10B shows a simulated optical path of the virtual display devicewithout the prism film in the embodiment shown in FIG. 6;

FIG. 11 shows a schematic diagram of an example backlight moduleprovided according to an embodiment of the present disclosure;

FIG. 12 schematically shows a schematic diagram of another examplebacklight module provided according to an embodiment of the presentdisclosure;

FIG. 13 is a schematic diagram of an example display device providedaccording to an embodiment of the present disclosure; and

FIG. 14 is a schematic diagram of another example display deviceprovided according to an embodiment of the present disclosure.

Throughout the various diagrams of these drawings, correspondingreference numerals indicate corresponding parts or features.

DETAILED DESCRIPTION

Various embodiments will be described in detail with reference to theaccompanying drawings, which are provided as exemplary examples of thepresent disclosure to enable those skilled in the art to implement thedisclosure. Notably, the figures and the examples below are not meant tolimit the scope of the present disclosure. Where certain elements of thepresent disclosure may be partially or fully implemented using knowncomponents, only those portions of such known components that arenecessary for an understanding of the present disclosure will bedescribed, and the detailed descriptions of other portions of such knowncomponents will be omitted so as not to obscure the present disclosure.Further, various embodiments encompass present and future knownequivalents to the components referred to herein by way of illustration.

When introducing the elements of this application and their embodiments,the terms “a”, “an”, “the” and “said” are intended to indicate thepresence of one or more elements, unless otherwise stated, the meaningof “multiple/a plurality of” is two or more, the terms “comprising”,“including”, “containing” and “having” are intended to be inclusive andindicate that there may be additional elements in addition to the listedelements, the terms “first”, “second”, “third”, etc. are used for thepurpose of description only, and are not to be construed as suggestingor implying relative importance and order of formation.

In virtual reality (VR) display technology, an image on a display screenis typically imaged by means of an imaging lens. During the imagingprocess, only part of the light from the display screen may pass throughthe lens and then be received by the user's eye. That is to say, onlypart of the light may be actually utilized, resulting in a large wasteof light energy. FIG. 1A shows a schematic diagram of an optical path(represented by thick arrows 11) of light emerging from a display screennot matching a desired optical path (represented by thin arrows 22) of aVR. FIG. 1B shows a schematic diagram of the optical path (representedby thick arrows 11) of light emerging from the display screen matchingthe desired optical path (represented by thin arrows 22) of the VR. Asshown in FIG. 1A, in an actual case, most of the light emerging from thedisplay screen 102 travels in a direction approximately perpendicular tothe display screen 102, as indicated by the thick arrows 11. Lightlocated near a center position 1 may enter the user's eye 106 afterpassing through the imaging lens 104, while most of the light near anedge position 2 cannot enter the user's eye 106 via the imaging lens104, thus causing waste of light. As shown in FIG. 1B, in the idealcase, the desired optical paths at different positions of the displayscreen 102 are different. Not only most of the light near the centerposition 1 may be received by the user's eye 106, but most of the lightnear the edge position 2 should also match the desired optical path 11to be received by the user's eye 106, which may improve the utilizationrate of light energy. Accordingly, it is desirable to provide an opticalstructure that may change the direction of light emerging from thedisplay screen in a manner that depends on the position of the displayscreen such that the optical path of the light emerging from the displayscreen matches the desired optical path of the VR.

It should be noted that, herein, the term “display device” refers to adevice capable of displaying a two-dimensional or three-dimensionalimage, which may include, for example, a backlight module, a displaypanel, and other optical films, the term “display panel” refers to aconstitute of the display device, and the term “display screen” refersto a screen of the display device capable of displaying an image, whichin embodiments of the present disclosure, may refer to a surface on adisplay image side of the entire display device. Herein, “light emergingfrom the display screen” refers to light that emerges from the surfaceof the display image side of the entire display panel, “light emergingfrom the display panel” and “light emerging from the display screen” mayhave the same meaning in the case where there is no additional filmlayer on the outer side of the display panel, but have different meaningin the case where there is an additional film layer (e.g., the prismfilm provided by the embodiment of the present disclosure) on the outerside of the display panel.

It should be noted that, in an embodiment of the present disclosure, thelight emerging from the respective light emerging points of the displayscreen, the display panel or the light guide plate may generally be acluster of light beams having a certain divergence angle. The primarylight energy of the cluster of light beams is typically concentratedover a small range of angles (e.g., from about 1° to about 20°). Forease of description, in embodiments of the present disclosure, thementioned descriptions referring to, for example, light or thedirection, angle, etc. of light generally mean the central light rays inthe cluster of light beams. However, this is not intended to limit thescope of the present disclosure to such particular central light rays,and those skilled in the art will appreciate that light within a rangeof angles on either side of the central light rays may be suitable forthe present disclosure.

An aspect of the present disclosure provides a prism film. Thestructural parameters of the prism film are designed such that lightemerging from the display screen may travel along a predeterminedtrajectory, such as along a desired optical path 2 of the VR, to takefull advantage of the light emerging from both the center and edgepositions of the display screen, thereby improving the utilization rateof light energy. The prism film may include a substrate and a pluralityof prisms on a surface of the substrate. Each prism has a triangularcross section, and has a first optical surface, a second opticalsurface, and a third optical surface that are perpendicular to thetriangular cross section. In an example embodiment, the first opticalsurface is parallel to the surface of the substrate. The first opticalsurface and the second optical surface form a first bottom angle of theprism, and the first optical surface and the third optical surface forma second bottom angle of the prism. At least one of the first bottomangles and the second bottom angles of the plurality of prisms graduallychanges.

As used herein, “gradually changing” may include the case ofmonotonously changing from one side of the substrate to the other sidethereof along a direction parallel to the surface of the substrate, andmay also include the case of first decreasing and then increasing fromone side of the substrate to the other side thereof. The term “surfaceof the substrate” refers to a surface of the substrate on which theprisms are provided.

FIG. 2 illustrates a cross-sectional view of a prism film providedaccording to an example embodiment of the present disclosure. In FIG. 2,an enlarged view of the prism 204 (located within the dashed oval belowthe prism film) is further illustrated. As shown in FIG. 2, the prismfilm 200 may include a substrate 202 and a plurality of prisms 204 onthe surface of the substrate 202. Each prism 204 has a triangular crosssection and has a first optical surface 2042, a second optical surface2044, and a third optical surface 2046 that are perpendicular to thetriangular cross section. The first optical surface 2042 is parallel tothe surface of the substrate 202. The first optical surface 2042 and thesecond optical surface 2044 form a first bottom angle α1 of the prism,and the first optical surface 2042 and the third optical surface 2046form a second bottom angle α3 of the prism.

FIG. 3 is a schematic diagram showing the effect of the prism filmprovided by the embodiment shown in FIG. 2 on parallel light incidentthereon. As shown in FIG. 3, after the parallel light is obliquelyincident on the prism film 200, the prisms on the prism film 200 mayadjust the direction of the outgoing light such that the outgoing lighttravels in a predetermined direction. In this embodiment, the pluralityof prisms 204 on the prism film 200 have different first and secondbottom angles. In a particular embodiment, the first bottom angles α1and the second bottom angles α3 of the plurality of prisms 204 may begradually increased along a direction parallel to a horizontal componentof light incident on the prisms 204 (as indicated by arrow 301 in FIG.3).

In an exemplary embodiment, the plurality of prisms 204 may be arrangedin parallel in a direction parallel to the surface of the substrate 202.However, this is not intended to limit the disclosure to this particulararrangement. Those skilled in the art may easily recognize how to adaptthe relevant parameters or conditions when employing differentarrangements. As an example, the plurality of prisms 204 may also bearranged in an array on the surface of the substrate 202.

FIGS. 4A and 4B schematically show two example optical paths of lighttransmitting through a prism film in the embodiment shown in FIG. 2,respectively. As shown in FIGS. 4A and 4B, the parameters of each prism204 (specifically, the first bottom angle α1 and the second bottom angleα3) may be configured such that light enters the prism 204 from thesecond optical surface 2044 and then is reflected by the third opticalsurface 2046 to the first optical surface 2042 and emerges from thefirst optical surface 2042 in a way of being deflected toward a centerof the substrate 202. An example method of determining a first bottomangle and a second bottom angle of a prism according to a predeterminedoptical path (a desired optical path) is described in detail below inconjunction with FIG. 4A. In the illustrated embodiment, α1, α2, and α3represent the first bottom angle, the apex angle, and the second bottomangle of the prism 204, respectively, n represents a refractive index ofthe prism, θ1 represents an angle facing the substrate 202 between adirection of the light incident on the second optical surface 2044 ofthe prism and a normal to the surface of the substrate 202°, θ2represents the complementary angle of θ1, θ3 and θ4 represent anincident angle and a refraction angle of the light at the second opticalsurface 2044 of the prism 204, respectively, θ5 and θ6 represent anincident angle and a reflection angle of light at the third opticalsurface 2046 of the prism 204, respectively, and θ7 and θ8 represent anincident angle and a refraction angle of the light at the first opticalsurface 2042 of the prism 204, respectively.

As shown in FIG. 4A, the following relationships may be obtainedaccording to the geometric relationship:

$\begin{matrix}{{{\theta \; 1} + {\theta \; 2}} = \frac{\pi}{2}} & (1) \\{{{\theta \; 3} + \frac{\pi}{2}} = {\pi - {\theta \; 2} - {\alpha \; 1}}} & (2) \\{{{\alpha 1} + {\alpha 2} + {\alpha \; 3}} = \pi} & (3) \\{{{\theta 4} + {\theta 5}} = {\alpha 2}} & (4) \\{{\frac{\pi}{2} - {\theta \; 7}} = {\pi - \left( {\frac{\pi}{2} - {\theta \; 6}} \right) - {\alpha \; 3}}} & (5)\end{matrix}$

Light incident on the second optical surface 2044 emerges at an angle θ8sequentially via the refraction by the second optical surface 2044, thereflection by the third optical surface 2046, and the refraction by thefirst optical surface 2042. According to the law of refraction and thelaw of reflection, the following relationships may be obtained:

sin θ3=n*sin θ4  (6)

θ5=θ6  (7)

n*sin θ7=sin θ8  (8)

Additionally, in order to enable light incident into each prism 204 tofollow the optical path shown in FIGS. 4A and 4B, i.e., light enteringthe prism 204 from the second optical surface 2044 is reflected by thethird optical surface 2046 and then emerges from the first opticalsurface 2042, the following relationship also needs to be satisfied:

$\begin{matrix}{{\frac{\pi}{2} - {\theta \; 4} - {\alpha 1}} < {\alpha \; 3}} & (9)\end{matrix}$

According to the above relationships (1)-(9), the followingrelationships among θ8, θ1, n, α1, and α3 may be obtained:

$\begin{matrix}{{\sin \; \theta \; 8} = {n*{\sin \left\lbrack {{\alpha 1} + {2*{\alpha 3}} - \pi + {\arcsin \; \frac{\sin \left( {{\theta \; 1} - {\alpha 1}} \right)}{n}}} \right\rbrack}}} & (10) \\{{{arc}\; \sin \; \frac{\sin \left( {{\theta \; 1} - {\alpha 1}} \right)}{n}} > {\frac{\pi}{2} - {\alpha \; 1} - {\alpha \; 3}}} & (11)\end{matrix}$

In an alternative embodiment, the structural parameters of the prism 204(specifically, the first bottom angle α1 and the second bottom angle α3)may also be configured such that light incident on the third opticalsurface 2046 is totally reflected on the third optical surface 2046, soas to improve the intensity of light emerging from the first opticalsurface 2042. In this case, it is also necessary to satisfy thefollowing relationship:

$\begin{matrix}{{\theta \; 5} > {\arcsin \; \frac{1}{n}}} & (12)\end{matrix}$

According to the above relationships (1)-(8) and (12), the followingrelationship may be further derived:

$\begin{matrix}{{\theta \; 5} = {{\pi - {\alpha 1} - {\alpha \; 3} - {\arcsin \; \frac{\sin \left( {{\theta \; 1} - {\alpha 1}} \right)}{n}}} > {\arcsin \; \frac{1}{n}}}} & (13)\end{matrix}$

According to the above relationships (10), (11), and (13), in the casewhere the angle θ1 between the direction of the light incident on thesecond optical surface 2044 of the prism 204 and the normal to thesurface of the substrate 202, the outgoing angle θ8 of light emergingfrom the first optical surface 2042 and the refractive index n of theprism 204 are known, the relationship between the first bottom angles α1and α3 may be derived.

In the illustrated embodiment, each prism 204 may have an isoscelestriangular cross section, i.e., α1=α3=α. In this configuration, thefirst bottom angle α1 and the second bottom angle α3 of the prism may bedetermined according to the above relationships (10), (11), and (13). Inthe case where θ1 is fixed, α1 and α3 change with θ8.

However, it should be noted that in the case where θ1 is small, lightentering the prism 204 from the second optical surface 2044 may not bereflected by the third optical surface 2046, but be directly incident onthe first optical surface 2042 from the second optical surface 2044 andemerges from the first optical surface 2042. In this case, thetravelling direction of the light emerging from the prism 204 does notconform to the desired optical path, which may also cause a certainamount of light energy loss. Therefore, in this embodiment, θ1 may beconfigured to have a larger angle, for example, 65°≤θ1≤85°. As anexample, such a prism film 200 may be applied to a backlight module of adisplay device because light emerging from a light guide plate of abacklight module generally has a large outgoing angle.

As already mentioned above, such a prism film 200 may be applied to avirtual reality display device. As an example, the prism film 200 may beprovided on the light outgoing side of the light guide plate of thevirtual reality display device. In this case, when the optical design isperformed, the outgoing angle θ8 of the light emerging from the firstoptical surface 2042 (which may be determined according to a desiredoptical path emerging from the display screen) may be predetermined suchthat the light emerging from the first optical surface 2042substantially conforms to the desired optical path as shown in FIGS. 1Aand 1B, in order to increase the utilization rate of light energy. Inthe virtual reality display device, it is generally also possible topredetermine the outgoing angle of light emerging from the light guideplate, i.e., θ1. Therefore, the first bottom angles α1 and the secondbottom angles α3 of the respective prisms may be determined according tothe above relationships (10), (11), and (13). In the case where theprisms are isosceles prisms, α1=α3. Thus, the respective prisms 204 onthe prism film may be designed based on the determined first bottomangles α1 and second bottom angles α3 such that the light emerging fromthe respective prisms substantially conform to the desired optical pathrequired in the virtual reality display device.

FIG. 5A shows a simulated optical path of a virtual reality displaydevice with the prism film of the embodiment shown in FIG. 2. In theexample shown in FIG. 5A, the prism film 200 may be provided on thelight outgoing side of the light guide plate of the VR display device,and the side of the prism film 200 provided with the prisms 204 facesthe light guide plate so that light emerging from the light guide platemay enter the prism 204 from the second optical surfaces 2044 of theprisms 204. In addition, the virtual reality display device in FIG. 5Amay also be designed in the following way:

the display screen 102 has a size of 62 mm, a center of the displayscreen 102 is located at 0 mm, and the interval between respectivepositions is 2 mm;

the angles of the light rays emerging from the display screen 102 atdifferent positions may be pre-designed according to the desired opticalpaths of the VR, assuming that the angles are equal to the outgoingangles θ8 of the light rays emerging from the first optical surfaces ofthe prisms, and the angles may be specifically listed in Table 1;

the angle θ1 between the direction of the light incident on the prisms204 and the normal to the surface of the substrate 202 is equal to 75°,which is equal to the outgoing angle of the light emerging from thedisplay screen 102;

the refractive index of the prisms 204 is n=1.49;

the pupil diameter of the eye 106 is set to be 8 mm, and

α1=α3=α.

Based on the above parameters and according to the above relationship(10), the first bottom angles α1 and the second bottom angles α3(α1=α3=α) at the respective positions may be calculated as listed inTable 1.

TABLE 1 The outgoing angles of the light rays emerging from the prismsat respective positions and the corresponding bottom angles of theprisms

−30 −28 −26 −24 −22 −20 −18 −16 −14 −12 −10 θ8 −19.3067 −18.5474−17.6181 −16.5616 −15.4055 −14.1717 −12.8779 −11.5386 −10.1647 −8.7642−7.3422 α 79.5 79 78.5 78 77.5 76.5 76 75 74.5 73.5 73

−8 −6 −4 −2 0 2 4 6 8 10 θ8 −5.9014 −4.4438 −2.9717 −1.4888 0 1.48882.9717 4.4438 5.9014 7.3422 α 72 71 70 69.5 68.5 67.5 67 66 65 64.5

12 14 16 18 20 22 24 26 28 30 θ8 8.7642 10.1647 11.5386 12.8779 14.171715.4055 16.5616 17.6181 18.5474 19.3067 α 63.5 62.5 62 61 60.5 60 5958.5 58 57.5

Based on the above configured parameters, the simulation results asshown in FIG. 5A may be obtained by establishing a model with simulationsoftware Lighttools. As can be seen from FIG. 5A, the light emergingfrom the display screen 102 (for example, light emerging from the edgeportion) may substantially match the desired optical path of the VR byusing the prism film 200 having the prisms 204 with varying bottomangles in the embodiment shown in FIG. 2, thereby improving theutilization rate of light energy.

FIG. 5B shows a simulated optical path of a virtual reality displaydevice with the prism film having the prisms of the same bottom angle.In FIG. 5B, a prism film having the same bottom angle (e.g., 56°) isused, and other parameters are the same as those in FIG. 5A. Obviously,in FIG. 5B, since light emerging from the edge of the display devicecannot enter the lens, and only light emerging at the central portionmay enter the user's eye 106 through the imaging lens, it will cause alarge waste of light energy. According to the simulation results in bothcases, the energy utilization rate of FIG. 5A is about 2.76 times thatof FIG. 5B.

FIG. 6 shows a cross-sectional view of a prism film provided accordingto another example embodiment of the present disclosure. In FIG. 6, anenlarged view of the prism 604 (inside the dashed oval below the prismfilm) is further illustrated. As shown in FIG. 6, the prism film 600includes a substrate 602 and a plurality of prisms 604 on a surface ofthe substrate 602. Each prism 604 has a right triangular cross-sectionand has a first optical surface 6042, a second optical surface 6044, anda third optical surface 6046 that are perpendicular to the righttriangular cross-section. The first optical surface 6042 is parallel tothe surface of the substrate 602. The first optical surface 6042 and thesecond optical surface 6044 form a first bottom angle α1 of the prism,and the first optical surface 6042 and the third optical surface 6046form a second bottom angle α1 of the prism (the second bottom angle is aright angle).

FIG. 7 is a schematic diagram showing the effect of the prism filmprovided by the embodiment shown in FIG. 6 on the parallel lightincident perpendicular thereon. As shown in FIG. 7, after the parallellight is incident perpendicularly onto the prism film 600, the prismfilm 600 may adjust the direction of the outgoing light such that theoutgoing light travels in a predetermined direction. In the embodimentshown in FIGS. 6 and 7, the first bottom angles α1 of the plurality ofprisms 604 may gradually decrease in a direction from the edge of thesubstrate 602 toward the center of the substrate 602 (as indicated byarrow 701 in FIG. 7), in order that the optical path of light emergingfrom the edge of the display screen substantially matches the desiredoptical path when such a prism film 600 is applied to a display device,thereby improving the utilization rate of light energy.

In the embodiments illustrated in FIGS. 6 and 7, the plurality of prisms604 may be arranged in parallel along a direction parallel to thesurface of the substrate 602 (as shown in FIG. 8A). In an alternativeembodiment, the plurality of prisms may be arranged in a way of aplurality of concentric circles (as shown in FIG. 8B). However, this isnot intended to limit the disclosure to these particular arrangements.Those skilled in the art may easily recognize how to adapt the relevantparameters or conditions when employing different arrangements.

FIG. 9 shows an example optical path of light transmission through theprism film in the embodiment shown in FIG. 6. As shown in the opticalpath 33 in FIG. 9 (indicated by solid arrow), the parameters of eachprism 602 (specifically, the first bottom angle α1) may be configuredsuch that light enters the prism from the first optical surface 6042, isincident onto the second optical surface 6044, is refracted by thesecond optical surface 6044, and then emerges from the second opticalsurface 6044 in a way of being deflected toward the center of thesubstrate.

An example method of determining a first bottom angle of a prism basedon a predetermined optical path (desired optical path) is described indetail below in conjunction with FIG. 9. In the illustrated embodiment,α1 and α2 represent a first bottom angle (first acute angle) and an apexangle (second acute angle) of the prism, respectively, n represents arefractive index of the prism, β1 and β2 represent an incident angle anda refraction angle of light at the first optical surface 6042,respectively, β3 and β4 represent an incident angle and a refractionangle of light at the second optical surface 6044, respectively, δrepresents an angle between light emerging from the second opticalsurface 6044 and a normal to the first optical surface 6042.

As shown in FIG. 9, the following relationships may be obtainedaccording to the geometric relationship:

$\begin{matrix}{{{\alpha 1} + {\alpha 2}} = \frac{\pi}{2}} & (14) \\{{{\beta 3} - {\beta 2} + {\alpha 2}} = \frac{\pi}{2}} & (15) \\{{{\alpha 1} + \delta} = {\beta 4}} & (16)\end{matrix}$

According to the optical path 33, the light incident on the firstoptical surface 6042 is sequentially refracted by the first opticalsurface 6042 and the second optical surface 6044 and then emerges fromthe second optical surface 6044 at the outgoing angle 134. According tothe law of refraction, the following relationships may be obtained:

sin β1=n*sin β2  (17)

n*sin β3=sin β4  (18)

Additionally, in order for light entering the prism from the firstoptical surface 6042 to emerge from the second optical surface 6044, itis desirable that the light does not satisfy the total reflectioncondition on the second optical surface 6044, i.e., the followingrelationship needs to be satisfied:

$\begin{matrix}{{\beta 3} < {\arcsin \; \frac{1}{n}}} & (19)\end{matrix}$

According to the above relationships (14)-(19), the followingrelationships among δ, β1, [[n]] n, and α1 may be obtained:

$\begin{matrix}{\delta = {{\arcsin \left\lbrack {n*{\sin \left( {{\alpha 1} + {\arcsin \; \frac{\sin \; {\beta 1}}{n}}} \right)}} \right\rbrack} - {\alpha 1}}} & (20) \\{{{\alpha 1} + {\arcsin \; \frac{\sin \; {\beta 1}}{n}}} < {\arcsin \; \frac{1}{n}}} & (21)\end{matrix}$

According to the above relationships (20) and (21), in the case wherethe incident angle β1 of the light incident on the first optical surface6042 of the prism 604, the angle δ between the light emerging from thesecond optical surface 6044 and the normal to the first optical surface6042 and the refractive index n of the prism 604 are known (assuming δis equal to the outgoing angle of the light emerging from the displayscreen), the first bottom angle α1 of the prism 604 may be calculated.

Further, as shown in FIG. 9, in the case where the incident angle β1 oflight incident on the first optical surface 6042 of the prism 604 is 0,that is, perpendicularly incident to the first optical surface 6042, thelight may be directly incident on the second optical surface 6044 fromthe first optical surface 6042 along the optical path 33. However, inthe case where the incident angle β1 of light incident on the firstoptical surface 6042 of the prism 604 is greater than 0, light near thethird optical surface 6046 may travel along the optical path 44(indicated by the broken line). Specifically, light entering the prismfrom the first optical surface 6042 is first incident on the thirdoptical surface 6046 and then incident on the second optical surface6044 after being reflected by the third optical surface 6046. In thelatter case, β1, δ, n, and α1 will not satisfy the above relationships(20) and (21), which will cause light energy loss to a certain degree.Therefore, in order to further improve the utilization rate of lightenergy, β1 may have a small angle, for example, 0°≤β1≤20°. However, thisis not intended to limit the scope of the present disclosure to thisparticular range of β1.

As an example, in the case where the prism film 600 in the embodimentshown in FIG. 6 is applied to a virtual reality display device, theprism film 600 may be provided on the light outgoing side of the displaypanel of the virtual display device as a part of the display device. Inthis case, the angle δ between the light emerging from the secondoptical surface 6044 and the normal to the first optical surface 6042may be pre-designed during optical design such that light emerging fromthe second optical surface 6044 substantially conforms to the desiredoptical path as shown in FIGS. 1A and 1B. That is, regardless ofemerging from the center of the display screen or from the edge of thedisplay screen, the light may enter the user's eye substantially via thelens, in order to improve the utilization rate of light energy. In thevirtual reality display device, it is generally also possible topredetermine the outgoing angle β1 of light emerging from the displaypanel (generally most of the light approximately perpendicularlyemerges), that is, β1=0. Therefore, in the case where the refractiveindex n of the prism 604 is known, the first bottom angle α1 of eachprism 604 may be determined according to the above relationships (20)and (21). Thus, respective prisms 604 on the prism film may be designedbased on the determined first bottom angle α1 such that the lightemerging from the respective prism 604 substantially conforms to thedesired optical path required in the virtual reality display device.

Alternatively, the prism film shown in FIG. 6 may be provided on thelight outgoing side of the light guide plate of the virtual realitydisplay device. In this case, those skilled in the art may easilyrecognize that the angle of the light emerging from the light guideplate may be adjusted by providing other optical components between theprism film and the light guide plate, to obtain a relatively small (31,so that the light is approximately perpendicularly incident to the firstoptical surface of the prism.

FIG. 10A shows a simulated optical path of a virtual reality displaydevice with the prism film of the embodiment shown in FIG. 6. In theexample shown in FIG. 10A, the prism film 600 may be provided on thelight outgoing side of the display panel of the VR display device, andthe side of the prism film 600 on which the prisms 604 are providedfaces away from the display panel such that light emerging from thedisplay panel may enter the prisms from the first optical surfaces 6042.In addition, the device in FIG. 10A may also be configured as follows:

the display screen 102 has a size of 62 mm, a center of the displayscreen 102 is located at 0 mm, and the interval between respectivepositions is 2 mm;

the angles of the light rays emerging from the display screen 102 atdifferent positions may be pre-designed according to the desired opticalpaths of the VR, assuming that the angles are equal to the angles δbetween the light rays emerging from the second optical surfaces of theprisms and the normal to the first optical surface, and the angles maybe specifically listed in Table 2;

light is incident perpendicularly to the first optical surface of eachprism, i.e., β1=0°.

the refractive index of the prism 204 is n=1.49.

According to the above relations (20) and (21), a (α1=α) at respectivepositions may be calculated as listed in Table 2.

TABLE 2 The outgoing angles of the light rays emerging from the prismsat respective positions and the corresponding bottom angles of theprisms

−30 −28 −26 −24 −22 −20 −18 −16 −14 −12 −10 δ −19.3067 −18.5474 −17.6181−16.5616 −15.4055 −14.1717 −12.8779 −11.5386 −10.1647 −8.7642 −7.3422 α31.2 30.4 29.4 28.2 26.8 25.2 23.4 21.4 19.2 16.9 14.4

−8 −6 −4 −2 0 2 4 6 8 10 δ −5.9014 −4.4438 −2.9717 −1.4888 0 1.48882.9717 4.4438 5.9014 7.3422 α 11.7 8.9 6 3 0 3 6 8.9 11.7 14.4

12 14 16 18 20 22 24 26 28 30 δ 8.7642 10.1647 11.5386 12.8779 14.171715.4055 16.5616 17.6181 18.5474 19.3067 α 16.9 19.2 21.4 23.4 25.2 26.828.2 29.4 30.4 31.2

Based on the above configured parameters, the simulation results asshown in FIG. 10A may be obtained by establishing a model withsimulation software Lighttools. As can be seen from FIG. 10A, the lightemerging from the display screen 102 may be substantially match thedesired optical path of the VR by using the prism film having the prismswith varying bottom angles in the embodiment shown in FIG. 6, therebyimproving the utilization rate of light energy.

FIG. 10B shows a simulated optical path of the virtual display devicewithout the prism film in the embodiment shown in FIG. 6. In FIG. 10B,the prism film in the embodiment shown in FIG. 6 is not applied on thelight outgoing side of the display panel, and other parameters are thesame as those in FIG. 10A. Obviously, in FIG. 10B, since light emergingat the edge of the display device cannot enter the lens, only lightemerging at the central portion may enter the user's eye through theimaging lens, it will cause a large waste of light energy. According tothe simulation results in both cases, the energy utilization rate ofFIG. 10A is about 2.76 times that of FIG. 10B.

To illustrate the particular effects, advantages, and feasibilities ofthe present disclosure, the use of the prism film described herein in avirtual reality display device is merely an exemplary application of aprism film that is not intended to limit the scope of the presentdisclosure to that particular application. With the embodiments of thepresent disclosure, when the prism film is applied to other scenes,those skilled in the art may easily recognize how to adapt relevantparameters and conditions. As an example, the prism film provided by theembodiments of the present disclosure may also be used to achieve somespecial display purposes, such as anti-peep.

Another aspect of the present disclosure provides a backlight module.The backlight module may include the prism film according to the presentdisclosure, such as the prism film according to one or more embodimentsdisclosed in detail above. Thus, for alternative embodiments of thebacklight module, reference may be made to the embodiments of the prismfilm.

FIG. 11 shows a schematic diagram of an example backlight moduleprovided according to an embodiment of the present disclosure. As shownin FIG. 11, the backlight module 1100 may include a light guide plate112 and a prism film 200 in the embodiment shown in FIG. 2, and theprism film 200 may be located on a light outgoing side of the lightguide plate 112.

In the embodiment shown in FIG. 11, the plurality of prisms 204 of theprism film 200 are arranged in parallel in a direction parallel to thesurface of the substrate 202. The first bottom angle and the secondbottom angle are configured such that light entering the prism from thesecond optical surface 2044 may be reflected toward the first opticalsurface 2042 by the third optical surface 2046 and then emerge from thefirst optical surface 2042 in a way of being deflected toward the centerof the substrate 202.

In the illustrated embodiment, the side of the prism film 200 providedwith the prisms 204 faces the light outgoing side of the light guideplate 112, and the outgoing angle of light emerging from the light guideplate 112 ranges from about 65° to about 85°.

FIG. 12 schematically shows a schematic diagram of another examplebacklight module provided according to an embodiment of the presentdisclosure. As shown in FIG. 12, the backlight module 1200 may include alight guide plate 112 and a prism film 600 in the embodiment shown inFIG. 6, and the prism film 600 may be located on the light outgoing sideof the light guide plate 112.

In the embodiment shown in FIG. 12, the prism 604 on the prism film 600has a right triangular cross-section, and the first bottom angle of theprism 604 is configured such that light entering the prism 604 from thefirst optical surface 6042 may be directly incident onto the secondoptical surface 6044, and emerges from the second optical surface in away of being deflected toward the center of the substrate 602.

In the illustrated embodiment, the side of the prism film 600 providedwith the prisms 604 faces away from the light outgoing side of the lightguide plate 112, and the incident angle of light incident onto the firstoptical surface 6042 of the prism 604 from the light guide plate 112ranges from about 0° to about 20°. As an example, other opticalcomponents may be provided between the light guide plate 112 and theprism film 600 in order to adjust the outgoing angle of the lightemerging from the light guide plate 112 so that the light is incident onthe first optical surface 6042 of the prism 604 at a relatively smallangle (for example, 0°).

The light guide plate provided by the embodiments shown in FIGS. 11 and12 may be applied to, for example, a virtual reality display device suchthat light emerging from the display screen may enter the user's eyethrough the imaging lens, thereby improving the utilization rate oflight energy.

Another aspect of the present disclosure provides a display device. Thedisplay device may include a prism film according to the presentdisclosure, such as a prism film according to one or more embodimentsdisclosed in detail above. Thus, for alternative embodiments of thedisplay device, reference may be made to embodiments of a prism film.

FIG. 13 is a schematic diagram of an example display device providedaccording to an embodiment of the present disclosure. As shown in FIG.13, the display device 1300 may include a backlight module or a lightguide plate 112, a display panel 131, and a prism film 200 in theembodiment shown in FIG. 2. In this embodiment, the prism film 200 maybe located between the light guide plate 112 and the display panel 131.

In the embodiment shown in FIG. 13, the plurality of prisms 204 may bearranged in a direction parallel to the surface of the substrate 202.The first bottom angle and the second bottom angle may be configuredsuch that light entering the prisms 204 from the second optical surface2044 may be reflected toward the first optical surface 2042 by the thirdoptical surface 2046, and then emerge from the first optical surface2042 in a way of being deflected toward the center of the substrate 202.In this embodiment, the side of the prism film 200 provided with theprisms 204 faces the light outgoing side of the light guide plate 112,and the outgoing angle of the light emerging from the light guide plate112 may range from about 65° to about 85°.

FIG. 14 is a schematic diagram of another example display deviceprovided according to an embodiment of the present disclosure. As shownin FIG. 14, the display device 1400 may include a backlight module or alight guide plate 112, a display panel 131, and a prism film 600 in theembodiment shown in FIG. 6. In this embodiment, the prism film 600 maybe located on the light outgoing side of the display panel 131.

In the embodiment shown in FIG. 14, the prism 604 on the prism film 600may have a right triangular cross section. The first bottom angle of theprism 604 is configured such that light entering the prism from thefirst optical surface 6042 may be incident directly onto the secondoptical surface 6044, and then emerge from the second optical surface6042 in a way of being deflected toward the center of the substrate 602.In this embodiment, the side of the prism film 600 provided with theprisms 604 faces away from the light outgoing side of the display panel131. The outgoing angle of light emerging from the display panel 131 mayrange from about 0° to about 20°.

The display device provided according to an embodiment of the presentdisclosure may be a virtual display device. With the display deviceprovided according to an embodiment of the present disclosure, lightemerging from the display device may travel according to predeterminedideal trajectories. Specifically, light emerging from the display devicemay enter the user's eye via the imaging lens of the virtual realitydevice, thereby improving the utilization rate of light energy.

It is to be understood that the term “about” used prior to a particularvalue herein means that the particular value can be tolerate a certainrange of error, and values within the range of error should be construedas falling within the scope of the present disclosure. As an example,“about 85°” may indicate an allowable error range of, for example, −1°to +1°, that is, any value within the range of 84° to 86° should fallwithin the range of values limited by the present disclosure.

As an alternative embodiment, the display device provided according toembodiments of the present disclosure may also be used in other scenes,for example, for the purpose of anti-peeping, and a better anti-peepingeffect may be achieved.

The foregoing description of the embodiment has been provided forpurpose of illustration and description. It is not intended to beexhaustive or to limit the application. Individual elements or featuresof a particular embodiment are generally not limited to that particularembodiment, but, where applicable, are interchangeable and can be usedin a selected embodiment, even if not specifically shown or described.The same may also be varied in many ways. Such variations are not to beregarded as a departure from the application, and all such modificationsare included within the scope of the application.

1. A prism film comprising a substrate and a plurality of prisms on asurface of the substrate, each of the plurality of prisms having atriangular cross section and having a first optical surface, a secondoptical surface, and a third optical surface that are perpendicular tothe triangular cross section, wherein the first optical surface isparallel to the surface of the substrate, wherein the first opticalsurface and the second optical surface form a first bottom angle,wherein the first optical surface and the third optical surface form asecond bottom angle, and wherein at least one of the first bottom angleand the second bottom angle of the plurality of prisms gradually changesin a direction parallel to the surface of the substrate.
 2. The prismfilm according to claim 1, wherein the plurality of prisms are arrangedin parallel in a direction parallel to the surface of the substrate, andwherein the first bottom angle and the second bottom angle areconfigured such that light entering the prism from the second opticalsurface is reflected toward the first optical surface by the thirdoptical surface, and then emerges from the first optical surface bybeing deflected toward a center of the substrate.
 3. The prism filmaccording to claim 2, wherein the direction is a direction of ahorizontal component of the light parallel to the surface of thesubstrate, and wherein the at least one of the first bottom angle andthe second bottom angle of the plurality of prisms gradually increasesin the direction.
 4. The prism film according to claim 3, wherein thefirst bottom angle and the second bottom angle are configured to satisfythe following relationship:${\sin \; \theta \; 8} = {n*{\sin \left\lbrack {{\alpha 1} + {2*{\alpha 3}} - \pi + {\arcsin \; \frac{\sin \left( {{\theta 1} - {\alpha 1}} \right)}{n}}} \right\rbrack}}$${\arcsin \; \frac{\sin \left( {{\theta 1} - {\alpha \; 1}} \right)}{n}} > {\frac{\pi}{2} - {\alpha 1} - {\alpha 3}}$wherein θ1 represents an angle, facing the substrate, between adirection of light incident on the prism and a normal to a surface ofthe substrate, n represents a refractive index of the prism, α1represents the first bottom angle, α3 indicates the second bottom angle,and θ8 represents an outgoing angle of light emerging from the firstoptical surface.
 5. The prism film according to claim 4, wherein thefirst bottom angle and the second bottom angle are configured such thatthe light incident to the third optical surface is totally reflected atthe third optical surface, and wherein the first bottom angle and thesecond bottom angle are further configured to satisfy the followingrelationship:${\theta 5} = {{\pi - {\alpha 1} - {\alpha 3} - {\arcsin \; \frac{\sin \left( {{\theta 1} - {\alpha 1}} \right)}{n}}} > {\arcsin \; \frac{1}{n}}}$wherein θ5 represents an incident angle of the light at the thirdoptical surface.
 6. The prism film according to claim 5, wherein thetriangular cross section is an isosceles triangular cross section. 7.The prism film according to claim 4, wherein 65°≤θ1≤Ξ°.
 8. The prismfilm according to claim 1, wherein the second bottom angle is a rightangle, and wherein the first bottom angle is configured such that lightentering the prism from the first optical surface is directly incidenton the second optical surface, and then emerges from the second opticalsurface by being deflected toward the center of the substrate.
 9. Theprism film according to claim 8, wherein the first bottom angle of theplurality of prisms gradually decreases from an edge of the substratetoward the center of the substrate.
 10. The prism film according toclaim 9, wherein the first bottom angle is configured to satisfy thefollowing relationship:$\delta = {{\arcsin \left\lbrack {n*{\sin \left( {{\alpha 1} + {\arcsin \; \frac{\sin \; {\beta 1}}{n}}} \right)}} \right\rbrack} - {\alpha \; 1}}$${{\alpha 1} + {\arcsin \; \frac{\sin \; {\beta 1}}{n}}} < {\arcsin \; \frac{1}{n}}$wherein δ represents an angle between light emerging from the secondoptical surface and a normal to the first optical surface, n representsa refractive index of the prism, α1 represents the first bottom angle,and β1 represents an incident angle of the light at the first opticalsurface.
 11. The prism film according to claim 10, wherein 0°≤β1≤20°.12. The prism film according to claim 8, wherein the plurality of prismsare arranged in parallel in a direction parallel to the surface of thesubstrate.
 13. The prism film according to claim 8, wherein theplurality of prisms are arranged in a form of a plurality of concentriccircles.
 14. A backlight module comprising a light guide plate and aprism film on a light outgoing side of the light guide plate accordingto claim
 1. 15. The backlight module according to claim 14, wherein theplurality of prisms are arranged in parallel along Rail the directionparallel to the surface of the substrate, wherein the first bottom angleand the second bottom angle are configured such that light entering theprism from the second optical surface is reflected toward the firstoptical surface by the third optical surface, and then emerges from thefirst optical surface by being deflected toward the center of thesubstrate, wherein a side of the prism film provided with the prisms isopposite to a light outgoing side of the light guide plate, and whereinan outgoing angle of light emerging from the light guide plate rangesfrom about 65° to about 85°.
 16. The backlight module according to claim14, wherein the triangular cross section is a right triangle crosssection, wherein the first bottom angle is configured such that lightentering the prism from the first optical surface is directly incidenton the second optical surface, and then emerges from the second opticalsurface by being deflected toward the center of the substrate, wherein aside of the prism film provided with the prisms faces away from a lightoutgoing side of the light guide plate, and wherein an outgoing angle ofthe light emerging from the light guide plate ranges from about 0° toabout 20°.
 17. A display device comprising a prism film according toclaim
 1. 18. The display device according to claim 17, furthercomprising a backlight module and a display panel, wherein the prismfilm is located between a light guide plate of the backlight module andthe display panel, wherein the plurality of prisms are arranged inparallel in a direction parallel to the surface of the substrate,wherein the first bottom angle and the second bottom angle areconfigured such that light entering the prism from the second opticalsurface is reflected toward the first optical surface by the thirdoptical surface, and then emerges from the first optical surface bybeing deflected toward the center of the substrate, wherein a side ofthe prism film provided with the prisms is opposite to a light outgoingside of the light guide plate, and wherein an outgoing angle of lightemerging from the light guide plate ranges from about 65° to about 85°.19. The display device according to claim 17, further comprising adisplay panel, wherein the prism film is located on a light outgoingside of the display panel, wherein the triangular cross section is aright triangle cross section, wherein the first bottom angle isconfigured such that light entering the prism from the first opticalsurface is directly incident on the second optical surface, and thenemerges from the second optical surface by being deflected toward thecenter of the substrate, wherein a side of the prism film provided withthe prisms faces away from a light outgoing side of the display panel,and wherein an outgoing angle of the light emerging from the light guideplate ranges from about 0° to about 20°.
 20. The display deviceaccording to claim 17, wherein the display device is a virtual realitydisplay device.